The third cutoff, introduced by Granda and Oliveros (GO)
[1]}, is the generalization of the Ricci scalar
[2]} in which we have \(L=(\beta \dot{H}+\alpha H^2)^{-1/2}\) 
where \(\alpha \)  and \(\beta \)  are constant, and therefore
\(\rho _D=3M_p^2(\alpha H^2+\beta \dot{H}),\) 
